a (lower bound), b (upper bound). We write X ~ U(a, b).(And f(x)=0 otherwise. The graph is a simple rectangle of height 1/(b-a) and width (b-a), so the area is 1).
μ (mu, the mean), σ² (sigma-squared, the variance). We write X ~ N(μ, σ²).This is how we use Z-tables to find probabilities for any Normal distribution.
λ (lambda, the "rate" of events; same λ as in the Poisson process).α (alpha) events have occurred in a Poisson process.α (alpha, the "shape" parameter, or number of events), λ (lambda, the "rate" parameter). We write X ~ Gamma(α, λ).Where Γ(α) (Gamma function) is a generalization of the factorial. Γ(n) = (n-1)! for integers. Γ(α) = ∫0∞ tα-1e-t dt.
α independent Exponential(λ) variables is a Gamma(α, λ) variable.α (alpha, shape), β (beta, shape). We write X ~ Beta(α, β).Where B(α, β) (Beta function) = Γ(α)Γ(β) / Γ(α+β).
θ (theta, location/median), γ (gamma, scale).The integrals ∫ x*f(x) dx and ∫ x²*f(x) dx do not converge. The M.G.F. also does not exist. The "tails" of the distribution are too "fat."
k (shape), λ (lambda, scale).μ (location/mean), b (scale).| Distribution | Parameters | Mean E[X] | Variance Var(X) |
|---|---|---|---|
| Uniform(a, b) | a, b | (a+b)/2 | (b-a)²/12 |
| Normal(μ, σ²) | μ, σ² | μ | σ² |
| Exponential(λ) | λ (rate) | 1/λ | 1/λ² |
| Gamma(α, λ) | α (shape), λ (rate) | α/λ | α/λ² |
| Beta(α, β) | α (shape), β (shape) | α / (α+β) | (αβ) / [ (α+β)²(α+β+1) ] |
| Cauchy(θ, γ) | θ (loc), γ (scale) | Undefined | Undefined |